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Title: Cherenkov Radiation (and other shocking waves).


1
Cherenkov Radiation (and other shocking waves).
Shock Waves May Confuse Birds Internal Compass
Perhaps also the ones of the fish?
http//www.newscientist.com/lastword/answers/lwa67
4bubbles.html http//www.pbs.org/wgbh/nova/barrier
/
2
The density effect in the energy loss is
intimately connected to the coherent response of
a medium to the passage of a relativistic
particle that causes the emission of Cherenkov
radiation.
Calculate the electromagnetic energy flow in a
cylinder of radius a around the track of the
particle.
a
Define
If a is in the order of atomic dimension and
laltlt1 we will then get the Fermi relation for
dE/dX with the density effect. If lagtgt1 , we
get (after some steps)
subscript 1 along particle velocity 2, 3
perpendicular to
If l has a positive real part ? the integrand
will vanish rapidly at large distances ? all
energy is deposited near the track If l is purely
imaginary ? the integrand is independent of a ?
some energy escapes at infinite as radiation ?
Cherenkov radiation and
or
and
we assume e real as from now on
3
Let us consider a particle that interacts with
the medium
Conservation of energy and momentum
The behavior of a photon in a medium is described
by the dispersion relation
Argon at normal density
W.W.M. Allison and P.R.S. Wright
RD/606-2000-January 1984
4
A particle with velocity b bv/c in a medium
with refractive index n nn(l) may emit light
along a conical wave front.
The angle of emission is given by
and the number of photons by
5
cos(q) 1/bn m p/bg Dm/m (Dp/p)2
(g2tgqDq)2½ set n 1.28 (C6F14) Dp/p2 51
0-4 Dq 15 mrad L 1 cm 1/l1 -1/l2 1/2200 -
1/1800 (l in A) with Q20
qmax 38.6 o bmin .78
p
K
p
6
Threshold Cherenkov Counter
Cherenkov gas
Particle with charge q velocity b
Spherical mirror
Flat mirror
Photon detector
To get a better particle identification, use more
than one radiator.
Positive particle identification
A radiator n1.0024 B radiator n1.0003
7
Directional Isochronous Selfcollimating Cherenkov
(DISC)
More general for an Imaging Detector
Cherenkov radiator nf(photon energy)
N photons Nf(b)
200nm 150
(n-1)106
b
Transformation Function
rf(b,n) D(r)f(resolution)
8
The light cone
The Cherenkov radiator
Q, b
The particle
9
http//banzai.msi.umn.edu/leonardo/
10
Detector
Focusing Mirror
Cherenkov media
e-
e
Proportional Chamber
g
g
g
Quartz Plate
e
e
e
E
Photon to Electron conversion gap
11
(No Transcript)
12
Particle Identification with the DELPHI RICHes
Liquid RICH
Cherenkov angle (mrad)
Gas RICH
p (GeV)
From data p from L K from F D p from Ko
http//delphiwww.cern.ch/delfigs/export/pubdet4.ht
ml
DELPHI, NIM A 378(1996)57
13
More beautiful pictures (which has next to
nothing to do with) Cherenkov radiation
ABB.com
14
An exact calculation of Transition Radiation is
complicated J. D. Jackson (bless him) and he
continues
A charged particle in uniform motion in a
straight line in free space does not radiate A
charged particle moving with constant velocity
can radiate if it is in a material medium and is
moving with a velocity greater than the phase
velocity of light in that medium (Cherenkov
radiation) There is another type of radiation,
transition radiation, that is emitted when a
charged particle passes suddenly from one medium
to another.
If elt1 no real photon can be emitted for an
infinite long radiator. Due to diffraction
broadening, sub-threshold emission of real
photons in thin radiators.
w02plasma frequency 2 ? (electron density)
If wgtgtw0
15
If wp2gtwp1 then Qmax ? g-1
Total radiated power S ? 10-2 g (eV) ? which is
a small number
16
Periodic radiator for Transition Radiation.
Coherent addition in point P
(-1)k The field amplitude for successive
interfaces alternate in sign A(Qk) Amplitude fk
w(R/c-t) phase factor
g 2 104 l1 25 mm l2 0.2 mm polypropylene -
air
Egorytchev, V Saveliev, V V Monte Carlo
simulation of transition radiation and electron
identification for HERA-B ITEP-99-11. - Moscow
ITEP , 17 May 1999.
17
Production with multi foils
saturation effect due to multi layer
Absorption in foils
w ? 10 keV
Conversion
X radiation
d-electron
MIP
Pulse Height
Threshold
t0
tT
M.L. Cerry et al., Phys. Rev. 10(1974)3594
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